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Toward understanding of Quark-Gluon Plasma in relativistic heavy ion collisions

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Toward understanding of Quark-Gluon Plasma in relativistic heavy ion collisions

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Toward understanding of Quark-Gluon Plasma in relativistic heavy ion collisions

Tetsufumi Hirano

Dept. of Physics

The University of Tokyo

Introduction heavy ion collisions

Basic Checks

Energy density

Chemical and kinetic equilibrium

Dynamics of Heavy Ion Collisions

Elliptic flow

Jet quenching

Summary and Outlook

Discussion

OUTLINEPhysics of the QGP heavy ion collisions

- Matter governed by QCD, not QED
- Frontier of high energy density/temperature
Toward an ultimate matter (Maximum energy density/temperature)

- Understanding the origin of matter which evolves with our universe
- Reproduction of QGP in H.I.C.
Reproduction of “early universe” on the Earth

History of the Universe heavy ion collisions ~ History of Matter

Quark Gluon Plasma

Hadronization

Nucleosynthesis

QGP study

Understanding

early universe

Little Bang! heavy ion collisions

front

view

Relativistic Heavy Ion Collider(2000-)

RHIC as a time machine!

STAR

side

view

STAR

Collision energy

Multiple production

(N~5000)

Heat

100 GeV per nucleon

Au(197×100)+Au(197×100)

BASIC CHECKS heavy ion collisions

Basic Checks (I): Energy Density heavy ion collisions

Bjorken(’83)

Bjorken energy density

total energy

(observables)

t: proper time

y: rapidity

R: effective transverse radius

mT: transverse mass

Critical Energy Density from Lattice heavy ion collisions

Stolen from Karsch(PANIC05);

Note that recent results seem to be Tc~190MeV

Centrality Dependence of Energy Density heavy ion collisions

Well above

ec from lattice

in central

collision at RHIC,

if assuming

t=1fm/c.

ec from lattice

PHENIX(’05)

CAVEATS (I) heavy ion collisions

- Just a necessary condition in the sense that temperature (or pressure) is not measured.
- How to estimate tau?
- If the system is thermalized, the actual energy density is larger due to pdV work.
- Boost invariant?
- Averaged over transverse area. Effect of thickness? How to estimate area?

Gyulassy, Matsui(’84) Ruuskanen(’84)

Basic Checks (II): Chemical Eq. heavy ion collisions

direct

Resonance decay

Two fitting parameters: Tch, mB

CAVEATS (II) heavy ion collisions

- Even e+e- or pp data can be fitted well!
See, e.g., Becattini&Heinz(’97)

- What is the meaning of fitting parameters? See, e.g., Rischke(’02),Koch(’03)
- Why so close to Tc?
- No chemical eq. in hadron phase!?
- Essentially dynamical problem!

Expansion rate Scattering rate

(Process dependent)

see, e.g., U.Heinz, nucl-th/0407067

Basic Checks (III): Radial Flow heavy ion collisions

Blast wave model (thermal+boost)

Driving force of flow

pressure gradient

Inside: high pressure

Outside: vacuum (p=0)

Sollfrank et al.(’93)

Spectrum for heavier particles

is a good place to see radial flow.

Spectral change is seen in AA! heavy ion collisions

Power law in pp & dAu

Convex to Power law

in Au+Au

- “Consistent” with thermal + boost picture
- Large pressure could be built up in AA collisions

O.Barannikova, talk at QM05

CAVEATS (III) heavy ion collisions

- Not necessary to be thermalized completely
- Results from hadronic cascade models.

- How is radial flow generated dynamically?
- Finite radial flow even in pp collisions?
- (T,vT)~(140MeV,0.2)
- Is blast wave reliable quantitatively?

- Consistency?
- Chi square minimum located a different point for f and W

- Flow profile? Freezeout hypersurface? Sudden freezeout?

Basic Checks heavy ion collisions Necessary Conditions to Study QGP at RHIC

- Energy density can be well above ec.
- Thermalized?

- “Temperature” can be extracted.
- Why freezeout happens so close to Tc?

- High pressure can be built up.
- Completely equilibrated?

Importance of systematic study based on dynamical framework

Dynamics of Heavy Ion Collisions heavy ion collisions

Dynamics of Heavy Ion Collisions heavy ion collisions

Freezeout

“Re-confinement”

Expansion, cooling

Thermalization

First contact

(two bunches of gluons)

Time scale

10fm/c~10-23sec

<<10-4(early universe)

Temperature scale 100MeV~1012K

y heavy ion collisions

Ncoll & NpartThickness function:

x

Gold nucleus:

r0=0.17 fm-3

R=1.12A1/3-0.86A-1/3

d=0.54 fm

Woods-Saxon nuclear density:

# of binary collisions

# of participants

sin = 42mb @200GeV

1－（survival probability）

Centrality heavy ion collisions

Npart and Ncoll as a function of

impact parameter

PHENIX: Correlation btw. BBC and ZDC signals

Elliptic Flow heavy ion collisions

What is Elliptic Flow? heavy ion collisions

Ollitrault (’92)

How does the system respond to spatial anisotropy?

No secondary interaction

Hydro behavior

y

f

x

INPUT

Spatial Anisotropy

2v2

Interaction among

produced particles

dN/df

dN/df

OUTPUT

Momentum Anisotropy

0

f

2p

0

f

2p

Time Evolution of a QGP Fluid heavy ion collisions

TH&Gyulassy(’06)

QGP

mixed

hadron

Anisotropy of energy density distribution

Anisotropy of “Momentum” distribution

v heavy ion collisions 2 from a Boltzmann simulation

Zhang et al.(’99)

ideal hydro limit

: Ideal hydro

v2

: strongly

interacting

system

b = 7.5fm

t(fm/c)

generated through secondary collisions

saturated in the early stage

sensitive to cross section (~1/m.f.p.~1/viscosity)

v2 is

Schematic Picture of Shear Viscosity heavy ion collisions

See, e.g. Danielewicz&Gyulassy(’85)

Assuming relativistic particles,

Perfect fluid:

l=1/sr 0

shear viscosity 0

Smearing of flow

Shear flow

Next time step

Basis of the Announcement heavy ion collisions

STAR(’02)

PHENIX(’03)

“Hydro limit”

response =

(output)/(input)

pT dependence

and mass ordering

Multiplicity dependence

Hydro results: Huovinen, Kolb, Heinz,…

It is found that they reproduce v2(pT) data accidentally.

T.Hirano and M.Gyulassy,Nucl.Phys.A769 (2006)71.

Recent Hydro Results heavy ion collisions from Our Group

Bottom-Up approach heavy ion collisions

- The first principle (QuantumChromo Dynamics)

- Inputs to phenomenology (lattice QCD)

Complexity

Non-linear interactions of gluons

Strong coupling

Dynamical many body system

Color confinement

- Phenomenology (hydrodynamics)

- Experimental data
- @ Relativistic Heavy Ion Collider
- ~150 papers from 4 collaborations
- since 2000

Why Hydrodynamics? heavy ion collisions

- Static
- EoS from Lattice QCD
- Finite T, m field theory
- Critical phenomena
- Chiral property of hadron

Once one accepts local

thermalization ansatz,

life becomes very easy.

Energy-momentum:

Conserved number:

- Dynamic Phenomena in HIC
- Expansion, Flow
- Space-time evolution of
- thermodynamic variables

Dynamics of Heavy Ion Collisions heavy ion collisions

Freezeout

“Re-confinement”

Expansion, cooling

Thermalization

First contact

(two bunches of gluons)

- Inputs in hydrodynamic simulations:
- Initial condition
- Equation of state
- Decoupling prescription

Centrality Dependence of v heavy ion collisions 2

TH et al. (’06).

- Discovery of “Large” v2 at RHIC
- v2 data are comparable with hydro results.
- Hadronic cascade cannot reproduce data.
- Note that, in v2 data, there exists eccentricity fluctuation which is not considered in model calculations.

Result from a hadronic cascade (JAM)

(Courtesy of M.Isse)

TH(’02); TH and K.Tsuda(’02); TH et al. (’06). heavy ion collisions

Pseudorapidity Dependence of v2QGP+hadron

- v2 data are comparable with hydro results again around h=0
- Not a QGP gas sQGP
- Nevertheless, large discrepancy in forward/backward rapidity
- See next slides

QGP only

h=0

h<0

h>0

Hadron Gas Instead of Hadron Fluid heavy ion collisions

T.Hirano and M.Gyulassy,Nucl.Phys.A769 (2006)71.

A QGP fluid surrounded

by hadronic gas

“Reynolds number”

QGP core

Matter proper part:

(shear viscosity)

(entropy density)

big

in Hadron

small

in QGP

QGP: Liquid (hydro picture)

Hadron: Gas (particle picture)

Importance of Hadronic heavy ion collisions “Corona”

- Boltzmann Eq. for hadrons instead of hydrodynamics
- Including viscosity through finite mean free path

QGP fluid+hadron gas

QGP+hadron fluids

QGP only

- Suggesting rapid increase of entropy density
- Deconfinement makes hydro work at RHIC!?
- Signal of QGP!?

T.Hirano et al.,Phys.Lett.B636(2006)299.

QGP Liquid + Hadron Gas Picture Works Well heavy ion collisions

20-30%

- Centrality dependence is ok
- Large reduction from pure hydro in small multiplicity events

Mass dependence is o.k.

Note: First result was obtained

by Teaney et al.

T.Hirano et al.,Phys.Lett.B636(2006)299.

QGP Liquid + Hadron Gas Picture Works Well (contd.) heavy ion collisions

hybrid model

AMPT

Adopted from S.J.Sanders

(BRAHMS) talk @ QM2006

How Fragile/Robust heavy ion collisions the Perfect Fluid Discovery is

1. Is mass ordering for v heavy ion collisions 2(pT) a signal of the perfect QGP fluid?

Pion

20-30%

Proton

Mass ordering comes from

rescattering effect. Interplay btw. radial and elliptic flows

Not a direct sign of the perfect QGP fluid

Mass dependence is o.k. from

hydro+cascade.

Why they shift oppositely? heavy ion collisions

pions

protons

v2(pT)

v2

<pT>

pT

v2 for protons can be negative

even in positive elliptic flow

must decrease with proper time

P.Huovinen et al.,PLB503,58(01)

TH and M.Gyulassy, NPA769,71(06)

Violation of Mass Ordering heavy ion collisions

Early decoupling from the system for phi mesons

Mass ordering is generated during hadronic evolution.

TH et al., arXiv:0710.5795[nucl-th].

2. Is viscosity really small in QGP? heavy ion collisions

- 1+1D Bjorken flow Bjorken(’83)
- Baym(’84)Hosoya,Kajantie(’85)Danielewicz,Gyulassy(’85)Gavin(’85)Akase et al.(’89)Kouno et al.(’90)…

(Ideal)

(Viscous)

h: shear viscosity (MeV/fm2), s : entropy density (1/fm3)

h/s is a good dimensionless measure

(in the natural unit) to see viscous effects.

Shear viscosity is small in comparison with entropy density!

TH and Gyulassy (’06) heavy ion collisions

A Probable Scenarioh: shear viscosity, s : entropy density

Kovtun,Son,Starinets(’05)

- Absolute value of viscosity

- Its ratio to entropy density

!

Rapid increase of entropy density can

make hydro work at RHIC.

Deconfinement Signal?!

Digression heavy ion collisions

[Pa] = [N/m2]

(Dynamical) Viscosity h:

~1.0x10-3 [Pa s] (Water20℃)

~1.8x10-5 [Pa s] (Air 20℃)

Kinetic Viscosity n=h/r:

~1.0x10-6 [m2/s] (Water20℃)

~1.5x10-5 [m2/s] (Air20℃)

hwater > hair BUT nwater < nair

Non-relativistic Navier-Stokes eq. (a simple form)

Neglecting external force and assuming incompressibility.

3. Is heavy ion collisions h/s enough?

- Reynolds number

Iso, Mori, Namiki (’59)

R>>1

Perfect fluid

- (1+1)D Bjorken solution

- Need to solve viscous fluid dynamics in (3+1)D
- Cool! But, tough!
- Causality problem

4. Boltzmann at work? heavy ion collisions

Molnar&Gyulassy(’00)

Molnar&Huovinen(’04)

25-30%

reduction

gluonic

fluid

s ~ 15 * spert !

Caveat 1: Where is the “dilute” approximation in Boltzmann

simulation? Is l~0.1fm o.k. for the Boltzmann description?

Caveat 2: Differential v2 is tricky. dv2/dpT~v2/<pT>.

Difference of v2 is amplified by the difference of <pT>.

Caveat 3: Hadronization/Freezeout are different.

5. Does v heavy ion collisions 2(pT) really tell us smallness of h/s in the QGP phase?

D.Teaney(’03)

- Not a result from dynamical calculation, but a “fitting” to data.
- No QGP in the model
- t0 is not a initial time, but a freeze-out time.
- Gs/t0 is not equal to h/s, but to 3h/4sT0t0 (in 1+1D).
- Being smaller T0 from pT dist., t0 should be larger (~10fm/c).

6. Is there model dependence in hydro calculations? heavy ion collisions

Novel initial conditions

from Color Glass Condensate

lead to large eccentricity.

Hirano and Nara(’04), Hirano et al.(’06)

Kuhlman et al.(’06), Drescher et al.(’06)

Need viscosity and/or

softer EoS in the QGP!

Summary heavy ion collisions

- Agreement btw. hydro and data comes from one particular modeling. (Glauber + ideal QGP fluid + hadron gas)
- IMO, still controversial for discovery of perfect fluid QGP.
- Check model dependences to obtain robust conclusion (and toward comprehensive understanding of the QGP from exp. data).

Heavy Ion Caf heavy ion collisions é

http://tkynt2.phys.s.u-tokyo.ac.jp/~hirano/hic/index.html